4.5 Article

In-plasma analysis of plasma-surface interactions

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REVIEW OF SCIENTIFIC INSTRUMENTS
卷 94, 期 8, 页码 -

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AIP Publishing
DOI: 10.1063/5.0130235

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During plasma processing of thin films and nanomaterials, various active species can interact with the sample simultaneously, such as reactive neutrals, positive ions, electrons, excited states, and photons. To monitor plasma-surface interactions, a new system with beams of neutral atoms, positive ions, UV photons, and a magnetron plasma source has been developed, equipped with in-plasma surface characterization tools like Rutherford Backscattering Spectrometer, Elastic Recoil Detector, and Raman spectroscopy system. This system provides time-resolved information on plasma-induced modification and can monitor atomic concentrations and Raman peak evolution during plasma deposition or etching.
During deposition, modification, and etching of thin films and nanomaterials in reactive plasmas, many active species can interact with the sample simultaneously. This includes reactive neutrals formed by fragmentation of the feed gas, positive ions, and electrons generated by electron-impact ionization of the feed gas and fragments, excited states (in particular, long-lived metastable species), and photons produced by spontaneous de-excitation of excited atoms and molecules. Notably, some of these species can be transiently present during the different phases of plasma processing, such as etching of thin layer deposition. To monitor plasma-surface interactions during materials processing, a new system combining beams of neutral atoms, positive ions, UV photons, and a magnetron plasma source has been developed. This system is equipped with a unique ensemble of in-plasma surface characterization tools, including (1) a Rutherford Backscattering Spectrometer (RBS), (2) an Elastic Recoil Detector (ERD), and (3) a Raman spectroscopy system. RBS and ERD analyses are carried out using a differentially pumped 1.7 MV ion beam line Tandetron accelerator generating a beam at grazing incidence. The ERD system is equipped with an absorber and is specifically used to detect H initially bonded to the surface; higher resolution of surface H is also available through nuclear reaction analysis. In parallel, an optical port facing the substrate is used to perform Raman spectroscopy analysis of the samples during plasma processing. This system enables fast monitoring of a few Raman peaks over nine points scattered on a 1.6 x 1.6 mm(2) surface without interference from the inherent light emitted by the plasma. Coupled to the various plasma and beam sources, the unique set of in-plasma surface characterization tools detailed in this study can provide unique time-resolved information on the modification induced by plasma. By using the ion beam analysis capability, the atomic concentrations of various elements in the near-surface (e.g., stoichiometry and impurity content) can be monitored in real-time during plasma deposition or etching. On the other hand, the evolution of Raman peaks as a function of plasma processing time can contribute to a better understanding of the role of low-energy ions in defect generation in irradiation-sensitive materials, such as monolayer graphene.

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